US5548427A - Switchable holographic apparatus - Google Patents

Switchable holographic apparatus Download PDF

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US5548427A
US5548427A US08/375,595 US37559595A US5548427A US 5548427 A US5548427 A US 5548427A US 37559595 A US37559595 A US 37559595A US 5548427 A US5548427 A US 5548427A
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polariser
retarder
pixels
switchable
polarisation
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Paul May
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Sharp Corp
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/29Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
    • G02F1/31Digital deflection, i.e. optical switching
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/32Holograms used as optical elements
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03HHOLOGRAPHIC PROCESSES OR APPARATUS
    • G03H1/00Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/137Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
    • G02F1/139Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent
    • G02F1/141Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent using ferroelectric liquid crystals
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2203/00Function characteristic
    • G02F2203/24Function characteristic beam steering
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03HHOLOGRAPHIC PROCESSES OR APPARATUS
    • G03H1/00Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
    • G03H1/0005Adaptation of holography to specific applications
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03HHOLOGRAPHIC PROCESSES OR APPARATUS
    • G03H1/00Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
    • G03H1/22Processes or apparatus for obtaining an optical image from holograms
    • G03H1/2294Addressing the hologram to an active spatial light modulator
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03HHOLOGRAPHIC PROCESSES OR APPARATUS
    • G03H2225/00Active addressable light modulator
    • G03H2225/20Nature, e.g. e-beam addressed
    • G03H2225/22Electrically addressed SLM [EA-SLM]

Definitions

  • the present invention relates to a switchable holographic apparatus.
  • a switchable holographic apparatus is suitable for use in optical computing, optical data storage and optical beam steering applications.
  • EP-A-451 681 discloses the use of an electrically addressable liquid crystal display for forming a hologram.
  • the hologram is created by controlling the individual pixels of the display so as to generate a suitable pattern of phase changes.
  • EP-A-449 164 also discloses use of a pixellated LCD to generate a hologram. Each pixel is individually controlled in order to generate the hologram.
  • EP-A-450 664 also discloses the use of a pixellated LCD to form a hologram in accordance with image data presented to the LCD.
  • Polarisation sensitive photopolymers may be used to form relatively complex retarder patterns, as reported by M. Schadt, K. Schmitt, V. Kozinkov and V. Chigrinov "Surface-induced parallel alignment of liquid crystals by linearly polymerised photopolymers" Jap journal of applied physics. Vol 31(1992) p2155-2164 and D. A. Yakolev, G. V. Simonenko, V. M. Kozenkov, V. G. Chigrinov and M. Schadt, "New Concept to Achieve Color LCDs with Linearly Photopolymerised (LPP) LCD-Substrates” in a paper presented to Eurodisplay 93, France.
  • a switchable holographic apparatus comprising a first polariser having a spatially varying direction of polarisation, a switchable retarder switchable between first and second states, and a second polariser, the switchable retarder being disposed in a radiation path between the first and second polarisers.
  • the radiation exiting from the second polariser is either substantially uniform or is spatially modulated in accordance with a pattern on the first polariser, depending on whether the retarder is in its first or second state.
  • the modulation may be phase modulation or amplitude modulation.
  • the first polariser is pixellated.
  • the first polariser comprises a plane polariser for polarising electromagnetic radiation along a first direction and a patterned retarder having a spatially varying retardation.
  • the spatially varying polarisation of the first polariser may be provided by regions thereof having different directions of polarisation. It is known, for example, from Schadt et al referred to hereinabove, that some linearly polymerisable photopolymers are dichroic within a restricted range of wavelengths. Such a photopolymer can be used to form a patterned polariser for use with light within that restricted range of wavelengths.
  • the patterned retarder is pixellated. Some or all of the pixels may be arranged to act as phase plates. Preferably the optical axis of each pixel is individually controllable.
  • the switchable retarder is a liquid crystal device.
  • the liquid crystal device is pixellated, each pixel of the liquid crystal device being associated with a plurality of pixels of the first polariser.
  • the electromagnetic radiation used is light.
  • light includes wavelengths falling within the infra-red, visible and ultra-violet regions of the spectrum.
  • an optical beam steering device comprising spatially modulated polarising means for providing a spatially modulated source of light comprising a plurality of regions producing plane polarised light polarised along one of a first direction and a second direction, an electrically controllable modulator having controllable birefringence for selectively controlling the directions of polarisation of the polarised light, so as to allow a hologram formed in the spatially modulated polarising means to be replayed, and a polariser arranged to receive light from the modulator and to transmit components of light polarised along a third direction.
  • FIG. 1 is a schematic diagram of an apparatus for forming a fixed phase or amplitude hologram
  • FIG. 2 is a side view of an apparatus constituting an embodiment of the present invention
  • FIG. 3 is a schematic view of an apparatus for forming a switchable phase hologram
  • FIG. 4 is a schematic view of an apparatus for forming a switchable amplitude hologram
  • FIG. 5 is a schematic diagram of an optical beam switcher constituting an embodiment of the present invention.
  • FIG. 6 is a schematic view of an alternate embodiment for forming a switchable hologram.
  • the apparatus shown in FIG. 1 comprises an input polariser 2, a patterned retarder 4 and an output polariser 6.
  • the input polariser provides linearly polarised light to the patterned retarder 4.
  • the light is vertically polarised, as indicated by the arrow 2a.
  • the patterned retarder 4 comprises a plurality of first and second pixels 4a,4b, respectively. Each pixel acts as a half-wave plate. The fast axis of retardation of each pixel is indicated by the arrows within each pixel.
  • the pixels 4a have their fast axis rotated by 22.5° in a clockwise direction with respect to the direction of polarisation of the polariser 2, whereas the pixels 4b have their fast axis rotated by 22.5° in an anti-clockwise direction with respect to the direction of polarisation of the polariser 2.
  • Each half wave plate introduces a ⁇ /2 phase shift between components of light parallel and perpendicular to the fast axis of the half wave plate.
  • the effect of each pixel is such that the light exiting each pixel has a polarisation at an angle with respect to the plane of polarised light incident on each pixel which is double the angle between the plane of polarisation of the incident polarised light and the fast axis of each pixel.
  • light emerging from the retarder 4 is polarised to an angle of ⁇ 45° with respect to the input polariser.
  • the direction of polarisation of the output polariser 6 may be perpendicular with respect to the input polariser 2 in order to form a phase modulated hologram or at ⁇ 45° with respect to the input polariser in order to form an amplitude modulated hologram.
  • FIG. 2 An electrically controllable holographic device is shown in FIG. 2.
  • An input polariser 2, a patterned retarder 4, which together with the input polariser 2 forms a first polariser, and an output polariser 6 are arranged as described with reference to FIG. 1.
  • a liquid crystal device 8 is interposed between the patterned retarder 4 and the output polariser 6.
  • Such an arrangement can be used to produce a phase hologram when the output polariser 6 is crossed with respect to the input polariser 2, as shown in FIG. 3.
  • the retarder 4 has a plurality of half wave plates having fast axes of retardation at an angle of ⁇ 22.5° with the plane of polarisation of the input polariser 2.
  • the liquid crystal device 8 such as a ⁇ cell, exhibits zero birefringence in the presence of a suitable control voltage.
  • the direction of polarisation of the light produced after passing through each pixel of the retarder 4 is unaffected by its passage through the liquid crystal device 8, i.e. it is still polarised at ⁇ 45° with respect to the input polariser 2, and hence at 45° and 135° with respect to the output polariser 6.
  • the output polariser resolves the light into components parallel to the plane of polarisation of the polariser. Thus a pattern of phase shifts of 0 and ⁇ radians are formed, and consequently the phase hologram is replayed.
  • the liquid crystal device is arranged to act as a half wave plate having its optic axis at an angle of 45° with respect to the direction of polarisation Of the input polariser.
  • the optic axis is parallel to one of the directions of polarisation of light from the pixels 4a, and perpendicular to the direction of polarisation of the light from the pixels 4b.
  • the action of a half wave plate is to produce light whose angle with the plane of polarisation of the incident light is double the angle that the incident light makes with the optic axis.
  • light from pixels 4a is unaffected, whereas light from the pixels 4b undergoes a phase shift of ⁇ radians, as shown in FIG. 3.
  • the light passing through the liquid crystal device 8 is now polarised at an angle of ⁇ 45° with respect to the direction of polarisation of the output polariser 6.
  • the polariser 6 resolves the light into components and transmits the component parallel to the direction of polarisation of the polariser.
  • the horizontal components of light due to the pixels 4a and 4b are in phase with each other. Thus there is no spatially modulated phase shift in the light exiting from the output polariser 6 and consequently the hologram is not visible.
  • a loss of 50% of the light occurs in both the "hologram on” and “hologram off” states.
  • Other retarder configurations are possible, but may result in unequal losses in the on and off states.
  • It is possible to simultaneously encode analogue amplitude information in addition to binary phase information by varying the optic axis of the pixels of the patterned retarder away from ⁇ 22.5°.
  • the phase hologram can still be controlled as described hereinabove, although in the off state the inverse of the amplitude modulation is observable. For example, if the optic axis of a pixel is 40° from the direction of polarisation of the input polariser, then the amplitude in the on state is 98%. In the off state, no phase modulation occurs, but transmission of the pixel is reduced to 2%.
  • an electrically or optically addressed ferroelectric liquid crystal device may be substituted for the patterned retarder 4.
  • the FLC acts as a reprogrammable patterned retarder.
  • the liquid crystal device 8 is then used to switch the hologram represented on the FLC on-and off, such an arrangement allows faster switching than is possible-by direct addressing of the FLC.
  • a FLC may be placed in series with the patterned retarder 4 and be arranged to act as a patterned switchable retarder, thus allowing the switching on and off of sub-holograms formed by the pixels within a region of the patterned retarder 4.
  • An amplitude modulated hologram may be formed by the arrangement illustrated in FIG. 4.
  • the output polariser 6 is parallel to the input polariser 2.
  • the liquid crystal device 8 is arranged to act, in the low voltage state, as a half wave plate, but the optic axis is now at an angle of 22.5°.
  • the light emerging from the pixels is at ⁇ 45°.
  • the LCD 8 is supplied with a relatively high voltage V switch , the LCD does not display birefringence, the polarisation of the light from the pixels is unaffected, and the vertical component of the light is selected by the output polariser 6.
  • the vertical component of the light is the same magnitude for light emanating from pixels 4a and pixels 4b.
  • the output from the output polariser is of substantially uniform intensity.
  • the liquid crystal device When a zero or low voltage is applied to the liquid crystal device, it functions as a half wave plate. Consequently the light emerging from the pixels 4b is rotated to be plane polarised parallel to the axis of the input polariser 2, whereas the light from pixels 4a is rotated to be plane polarised perpendicular to the axis of the input polariser 2. Thus only light from the pixels 4b is transmitted by the output polariser 6, and consequently the amplitude modulation is replayed.
  • quarter wave patterned retarders having the fast axes of each type of pixel perpendicular to one another and the liquid crystal device 8 arranged to act as a switchable quarter wave plate having its fast axis parallel to one of the groups of pixels of the patterned retarder.
  • the device could have either parallel or crossed input and output polarisers and the order of the liquid crystal device and the patterned retarder may be interchanged.
  • a sequence of such switchable holographic elements may be formed by placing the devices in series, thereby giving rise to 2"different holograms, where n is the number of devices, and may typically be 3 or 4.
  • n is the number of devices, and may typically be 3 or 4.
  • the devices need to be in close contact, or alternatively the holograms require relatively long working distances.
  • FIG. 5 shows a beam switching device comprising: an input polariser 2, a patterned retarder 4, a liquid crystal device 8, and an output polariser 6, as described hereinabove; and an input fibre 10, a lens 12 and first and second output fibres 14 and 16.
  • Light from the input fibre (at position A) is collected by the lens 12 and imaged towards a point B at an end of the first output fibre 14.
  • the polarisers 2,6, the patterned retarder 4 and the liquid crystal device 8 are in the optical path between the lens 12 and the output fibre 14.
  • the holographic image is arranged to steer the beam away from point B and towards point C at the end of the second output fibre 16.
  • the hologram is designed to provide both a beam steering and a focusing action, i.e. it is an off-centre zone plate.
  • the focal length of the zone plate may typically be between 1 mm and 1 meter and may be optimised for particular wavelengths.
  • Such a zone plate would be difficult to create using a directly addressed liquid crystal device, because of the problems of addressing concentric circles of elements, and also because of the spatial resolution that would be required for simulating the shortest focal length lenses.
  • FIG. 6 shows an alternate embodiment of a switchable holographic apparatus.
  • the spatially varying polarisation of the first polariser is provided by a patterned polariser instead of the combined plane polariser and patterned retarder having a spatially varying retardation.
  • a patterned polariser instead of the combined plane polariser and patterned retarder having a spatially varying retardation.
  • some linearly polymerisable photopolymers are dichroic within a restricted range of wavelengths.
  • Such a photopolymer can be used to form a patterned polariser for use with light within that restricted range of wavelengths.
  • Such devices may be combined in series or in parallel to provide a diverse and complex pattern of holographic images to be rapidly selected.
  • Such devices may be used as switchable Fourier plane filters for optical computing applications, optical data storage, and beam steering for optical disc and telecommunication applications.

Abstract

A switchable holographic device which includes a first polarizer having a spatially varying direction of polarization. The device also includes a liquid crystal device arranged to act as a controllable phase plate, the liquid crystal device having a predetermined phase shift in one state and substantially no birefringent activity in another state. The liquid crystal device is thus controllable to selectively alter the polarization of at least some of the radiation passing therethrough or to have substantially no optical activity. An output polarizer receives the radiation from the liquid crystal device so that, depending on the state of the liquid crystal device, the hologram is replayed or not replayed.

Description

The present invention relates to a switchable holographic apparatus. Such a device is suitable for use in optical computing, optical data storage and optical beam steering applications.
D. C. O'Brien, T. D. Wilkinson, R. J. Mears, and W. A. Crossland, in a paper entitled "Generalised dynamic holographic interconnects using spatial light modulators", Light modulators and applications, OSA meeting, Palm Springs, March 1993, disclose a computer generated hologram using a ferroelectric liquid crystal spatial light modulator (SLM) to provide binary phase modulation. The SLM is illuminated with a collimated beam of light, and the light emerging from the SLM is transformed using a lens so as to replay the hologram. The phase changes provided by the SLM form the hologram. In order to replay relatively complex holograms, and especially holograms having irregular dot patterns, each element of the SLM needs to be addressed in parallel. This may impose severe pin out requirements on the SLM and result in bulky systems.
EP-A-451 681 discloses the use of an electrically addressable liquid crystal display for forming a hologram. The hologram is created by controlling the individual pixels of the display so as to generate a suitable pattern of phase changes.
EP-A-449 164 also discloses use of a pixellated LCD to generate a hologram. Each pixel is individually controlled in order to generate the hologram.
EP-A-450 664 also discloses the use of a pixellated LCD to form a hologram in accordance with image data presented to the LCD.
Polarisation sensitive photopolymers may be used to form relatively complex retarder patterns, as reported by M. Schadt, K. Schmitt, V. Kozinkov and V. Chigrinov "Surface-induced parallel alignment of liquid crystals by linearly polymerised photopolymers" Jap journal of applied physics. Vol 31(1992) p2155-2164 and D. A. Yakolev, G. V. Simonenko, V. M. Kozenkov, V. G. Chigrinov and M. Schadt, "New Concept to Achieve Color LCDs with Linearly Photopolymerised (LPP) LCD-Substrates" in a paper presented to Eurodisplay 93, Strasbourg.
According to a first aspect of the present invention, there is provided a switchable holographic apparatus, comprising a first polariser having a spatially varying direction of polarisation, a switchable retarder switchable between first and second states, and a second polariser, the switchable retarder being disposed in a radiation path between the first and second polarisers.
It is thus possible to provide a device in which the radiation exiting from the second polariser is either substantially uniform or is spatially modulated in accordance with a pattern on the first polariser, depending on whether the retarder is in its first or second state. The modulation may be phase modulation or amplitude modulation.
Advantageously the first polariser is pixellated.
Preferably the first polariser comprises a plane polariser for polarising electromagnetic radiation along a first direction and a patterned retarder having a spatially varying retardation.
Alternatively, the spatially varying polarisation of the first polariser may be provided by regions thereof having different directions of polarisation. It is known, for example, from Schadt et al referred to hereinabove, that some linearly polymerisable photopolymers are dichroic within a restricted range of wavelengths. Such a photopolymer can be used to form a patterned polariser for use with light within that restricted range of wavelengths.
Preferably the patterned retarder is pixellated. Some or all of the pixels may be arranged to act as phase plates. Preferably the optical axis of each pixel is individually controllable.
Preferably the switchable retarder is a liquid crystal device.
Advantageously the liquid crystal device is pixellated, each pixel of the liquid crystal device being associated with a plurality of pixels of the first polariser.
Advantageously, in use, the electromagnetic radiation used is light. In this context, light includes wavelengths falling within the infra-red, visible and ultra-violet regions of the spectrum.
According to a second aspect of the present invention, there is provided an optical beam steering device, comprising spatially modulated polarising means for providing a spatially modulated source of light comprising a plurality of regions producing plane polarised light polarised along one of a first direction and a second direction, an electrically controllable modulator having controllable birefringence for selectively controlling the directions of polarisation of the polarised light, so as to allow a hologram formed in the spatially modulated polarising means to be replayed, and a polariser arranged to receive light from the modulator and to transmit components of light polarised along a third direction.
The present invention will be further described, by way of example, with reference to the accompanying drawings, in which:
FIG. 1 is a schematic diagram of an apparatus for forming a fixed phase or amplitude hologram;
FIG. 2 is a side view of an apparatus constituting an embodiment of the present invention;
FIG. 3 is a schematic view of an apparatus for forming a switchable phase hologram;
FIG. 4 is a schematic view of an apparatus for forming a switchable amplitude hologram; and
FIG. 5 is a schematic diagram of an optical beam switcher constituting an embodiment of the present invention.
FIG. 6 is a schematic view of an alternate embodiment for forming a switchable hologram.
The apparatus shown in FIG. 1 comprises an input polariser 2, a patterned retarder 4 and an output polariser 6. The input polariser provides linearly polarised light to the patterned retarder 4. In this example, the light is vertically polarised, as indicated by the arrow 2a. The patterned retarder 4 comprises a plurality of first and second pixels 4a,4b, respectively. Each pixel acts as a half-wave plate. The fast axis of retardation of each pixel is indicated by the arrows within each pixel. The pixels 4a have their fast axis rotated by 22.5° in a clockwise direction with respect to the direction of polarisation of the polariser 2, whereas the pixels 4b have their fast axis rotated by 22.5° in an anti-clockwise direction with respect to the direction of polarisation of the polariser 2. Each half wave plate introduces a λ/2 phase shift between components of light parallel and perpendicular to the fast axis of the half wave plate. The effect of each pixel is such that the light exiting each pixel has a polarisation at an angle with respect to the plane of polarised light incident on each pixel which is double the angle between the plane of polarisation of the incident polarised light and the fast axis of each pixel. Thus light emerging from the retarder 4 is polarised to an angle of ±45° with respect to the input polariser. The direction of polarisation of the output polariser 6 may be perpendicular with respect to the input polariser 2 in order to form a phase modulated hologram or at ±45° with respect to the input polariser in order to form an amplitude modulated hologram.
An electrically controllable holographic device is shown in FIG. 2. An input polariser 2, a patterned retarder 4, which together with the input polariser 2 forms a first polariser, and an output polariser 6 are arranged as described with reference to FIG. 1. Additionally a liquid crystal device 8 is interposed between the patterned retarder 4 and the output polariser 6. Such an arrangement can be used to produce a phase hologram when the output polariser 6 is crossed with respect to the input polariser 2, as shown in FIG. 3. As before, the retarder 4 has a plurality of half wave plates having fast axes of retardation at an angle of ±22.5° with the plane of polarisation of the input polariser 2. The liquid crystal device 8, such as a π cell, exhibits zero birefringence in the presence of a suitable control voltage. The direction of polarisation of the light produced after passing through each pixel of the retarder 4 is unaffected by its passage through the liquid crystal device 8, i.e. it is still polarised at ±45° with respect to the input polariser 2, and hence at 45° and 135° with respect to the output polariser 6. The output polariser resolves the light into components parallel to the plane of polarisation of the polariser. Thus a pattern of phase shifts of 0 and π radians are formed, and consequently the phase hologram is replayed.
In the low applied voltage state, the liquid crystal device is arranged to act as a half wave plate having its optic axis at an angle of 45° with respect to the direction of polarisation Of the input polariser. Thus the optic axis is parallel to one of the directions of polarisation of light from the pixels 4a, and perpendicular to the direction of polarisation of the light from the pixels 4b. As noted hereinabove, the action of a half wave plate is to produce light whose angle with the plane of polarisation of the incident light is double the angle that the incident light makes with the optic axis. Thus light from pixels 4a is unaffected, whereas light from the pixels 4b undergoes a phase shift of π radians, as shown in FIG. 3. The light passing through the liquid crystal device 8 is now polarised at an angle of ±45° with respect to the direction of polarisation of the output polariser 6. The polariser 6 resolves the light into components and transmits the component parallel to the direction of polarisation of the polariser. The horizontal components of light due to the pixels 4a and 4b are in phase with each other. Thus there is no spatially modulated phase shift in the light exiting from the output polariser 6 and consequently the hologram is not visible.
For the arrangement described hereinabove, a loss of 50% of the light occurs in both the "hologram on" and "hologram off" states. Other retarder configurations are possible, but may result in unequal losses in the on and off states. It is possible to simultaneously encode analogue amplitude information in addition to binary phase information by varying the optic axis of the pixels of the patterned retarder away from ±22.5°. The phase hologram can still be controlled as described hereinabove, although in the off state the inverse of the amplitude modulation is observable. For example, if the optic axis of a pixel is 40° from the direction of polarisation of the input polariser, then the amplitude in the on state is 98%. In the off state, no phase modulation occurs, but transmission of the pixel is reduced to 2%.
In an alternative arrangement, an electrically or optically addressed ferroelectric liquid crystal device (FLC) may be substituted for the patterned retarder 4. The FLC acts as a reprogrammable patterned retarder. The liquid crystal device 8 is then used to switch the hologram represented on the FLC on-and off, such an arrangement allows faster switching than is possible-by direct addressing of the FLC.
As a further alternative, a FLC may be placed in series with the patterned retarder 4 and be arranged to act as a patterned switchable retarder, thus allowing the switching on and off of sub-holograms formed by the pixels within a region of the patterned retarder 4.
An amplitude modulated hologram may be formed by the arrangement illustrated in FIG. 4. The output polariser 6 is parallel to the input polariser 2. Additionally, the liquid crystal device 8 is arranged to act, in the low voltage state, as a half wave plate, but the optic axis is now at an angle of 22.5°. As before, the light emerging from the pixels is at ±45°. When the LCD 8 is supplied with a relatively high voltage Vswitch, the LCD does not display birefringence, the polarisation of the light from the pixels is unaffected, and the vertical component of the light is selected by the output polariser 6. The vertical component of the light is the same magnitude for light emanating from pixels 4a and pixels 4b. Thus the output from the output polariser is of substantially uniform intensity.
When a zero or low voltage is applied to the liquid crystal device, it functions as a half wave plate. Consequently the light emerging from the pixels 4b is rotated to be plane polarised parallel to the axis of the input polariser 2, whereas the light from pixels 4a is rotated to be plane polarised perpendicular to the axis of the input polariser 2. Thus only light from the pixels 4b is transmitted by the output polariser 6, and consequently the amplitude modulation is replayed.
Other arrangements are possible, such as quarter wave patterned retarders having the fast axes of each type of pixel perpendicular to one another and the liquid crystal device 8 arranged to act as a switchable quarter wave plate having its fast axis parallel to one of the groups of pixels of the patterned retarder. The device could have either parallel or crossed input and output polarisers and the order of the liquid crystal device and the patterned retarder may be interchanged.
A sequence of such switchable holographic elements may be formed by placing the devices in series, thereby giving rise to 2"different holograms, where n is the number of devices, and may typically be 3 or 4. In order to be additive, the devices need to be in close contact, or alternatively the holograms require relatively long working distances.
FIG. 5 shows a beam switching device comprising: an input polariser 2, a patterned retarder 4, a liquid crystal device 8, and an output polariser 6, as described hereinabove; and an input fibre 10, a lens 12 and first and second output fibres 14 and 16. Light from the input fibre (at position A) is collected by the lens 12 and imaged towards a point B at an end of the first output fibre 14. The polarisers 2,6, the patterned retarder 4 and the liquid crystal device 8 are in the optical path between the lens 12 and the output fibre 14. When the liquid crystal device is switched so as to replay the hologram encoded on the patterned retarder 4, the holographic image is arranged to steer the beam away from point B and towards point C at the end of the second output fibre 16. The hologram is designed to provide both a beam steering and a focusing action, i.e. it is an off-centre zone plate. The focal length of the zone plate may typically be between 1 mm and 1 meter and may be optimised for particular wavelengths.
Such a zone plate would be difficult to create using a directly addressed liquid crystal device, because of the problems of addressing concentric circles of elements, and also because of the spatial resolution that would be required for simulating the shortest focal length lenses.
FIG. 6 shows an alternate embodiment of a switchable holographic apparatus. In this case, the spatially varying polarisation of the first polariser is provided by a patterned polariser instead of the combined plane polariser and patterned retarder having a spatially varying retardation. It is known, for example, from Schadt et al. referred to hereinabove, that some linearly polymerisable photopolymers are dichroic within a restricted range of wavelengths. Such a photopolymer can be used to form a patterned polariser for use with light within that restricted range of wavelengths.
It is thus possible to provide a device in which a highly complex holographic image is pre-recorded on a patterned retarder, and in which a liquid crystal device is easily and quickly controlled to selectively replay the image. Such devices may be combined in series or in parallel to provide a diverse and complex pattern of holographic images to be rapidly selected. Such devices may be used as switchable Fourier plane filters for optical computing applications, optical data storage, and beam steering for optical disc and telecommunication applications.

Claims (25)

What is claimed is:
1. A switchable holographic apparatus, comprising:
a first polariser having a spatially varying direction of polarisation,
a switchable retarder switchable between first and second states, and
a second polariser, wherein
the switchable retarder is disposed in a radiation path between the first and second polarisers,
the first polariser comprises a plurality of first pixels having respective directions of polarisation arranged at a first angle to a first direction, and
the switchable retarder is pixellated and each pixel of the switchable retarder is associated with a plurality of pixels of the first polariser.
2. An apparatus according to claim 1, wherein the first polariser further comprises a plurality of second pixels having respective directions of polarisation arranged at a second angle to the first direction.
3. An apparatus according to claim 2, wherein the first and second angles are of equal magnitude and opposite sign.
4. An apparatus according to claim 1, wherein the first polariser comprises a plane polariser for polarising electromagnetic radiation along a first direction and a patterned retarder having a spatially varying retardation.
5. An apparatus according to claim 4, wherein the patterned retarder comprises a plurality of first pixels having respective optic axes arranged at a first angle to the first direction.
6. An apparatus according to claim 5, wherein the patterned retarder further comprises a plurality of second pixels having respective optic axes arranged at a second angle to the first direction.
7. An apparatus according to claim 6, wherein the first and second angles are of equal magnitude and opposite sign.
8. An apparatus according to claim 5, wherein the pixels are arranged to act as phase-plates.
9. An apparatus according to claims 4, wherein the patterned retarder is a pixellated ferroelectric liquid crystal device, the pixels being controllable so as to form a programmable retarder.
10. An apparatus according to claim 1, wherein the switchable retarder exhibits substantially no birefringence in the first state and acts as a phase plate in the second state.
11. An apparatus according to claim 1, wherein the switchable retarder is arranged, when in the second state, to act as a half wave plate.
12. An apparatus according to claim 6, wherein the switchable retarder exhibits substantially no birefringence in the first state and acts as a half wave plate in the second state, and the first and second pixels are arranged to act as half wave plates.
13. An apparatus according to claim 12, wherein the direction of polarisation of the second polariser is crossed with respect to that of the plane polariser, the switchable retarder has an optic axis at substantially 45 degrees with respect to the first direction and the apparatus is arranged to replay a phase hologram.
14. An apparatus according to claim 12, wherein the direction of polarisation of the second polariser is parallel to that of the plane polariser, the switchable retarder has an optic axis at substantially 22.5 degrees with respect to the first direction and the apparatus is arranged to replay an amplitude hologram.
15. An apparatus according to claim 12, wherein the optic axes of the first and second pixels are oriented at an angle of +22.5 degrees and -22.5 degrees with respect to the first direction, respectively.
16. An apparatus according to claim 6, wherein the switchable retarder exhibits substantially no birefringence in the first state and acts as a phase plate in the second state, and the first and second pixels are arranged to act as quarter wave plates, the optic axes of the first and second pixels are perpendicular to one another and the switchable retarder is arranged, when in the second state, to act as a quarter wave plate having an optic axis substantially parallel to the optic axis of the first pixels.
17. An apparatus according to claim 16, wherein the direction of polarisation of the second polariser is crossed or parallel with that of the plane polariser.
18. An apparatus according to claim 4, wherein the patterned retarder is formed of a photopolymer.
19. An apparatus according to claim 1, wherein the switchable retarder is a liquid crystal device.
20. An apparatus according to claim 19, wherein the switchable retarder is a π cell.
21. An apparatus according to claim 1, wherein the switchable retarder is pixellated.
22. An apparatus according to claim 5, wherein the switchable retarder is pixellated and each pixel of the switchable retarder is associated with a plurality of pixels of the first polariser.
23. A beam steering apparatus comprising a switchable holographic device comprising;
a first polariser having a spatially varying direction of polarisation,
a switchable retarder switchable between first and second states, and
a second polariser, wherein
the switchable retarder is disposed in a radiation path between the first and second polarisers,
the first polariser comprises a plurality of first pixels having respective directions of polarisation arranged at a first angle to a first direction, and
the switchable retarder is pixellated and each pixel of the switchable retarder is associated with a plurality of pixels of the first polariser.
24. An optical beam steering apparatus, comprising:
spatially modulated polarising means for providing a spatially modulated source of light comprising a plurality of regions producing plane polarised light polarised along one of a first direction and a second direction,
an electrically controllable modulator having controllable birefringence for selectively controlling the directions of polarisation of the polarised light, so as to allow a hologram formed in the spatially modulated polarising means to be replayed, and
a polariser arranged to receive light from the modulator and to transmit components of light polarised along a third direction,
wherein the electrically controllable modulator is pixellated and each pixel of the electrically controllable modulator is associated with the plurality of regions of the spatially modulated polarising means.
25. An apparatus according to claim 1, wherein said first polariser is a patterned polariser.
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Cited By (50)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5745203A (en) * 1996-03-28 1998-04-28 Motorola, Inc. Liquid crystal display device including multiple ambient light illumination modes with switchable holographic optical element
US5784139A (en) * 1991-07-26 1998-07-21 Rolic Ag Image display device
US5946098A (en) * 1997-12-23 1999-08-31 J.A. Woollam Co. Inc. Optical elements for use in spectroscopic ellipsometer and polarimeter systems
US6084674A (en) * 1999-01-04 2000-07-04 J. A. Woollam Co., Inc. Parallelogram shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6100981A (en) * 1999-01-04 2000-08-08 J.A. Woollam Co. Inc. Dual horizontally oriented triangle shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6118537A (en) * 1999-01-04 2000-09-12 J. A. Woollam Co. Inc. Multiple tipped berek plate optical retarder elements for use in spectroscopic ellipsometer and polarimeter systems
US6137618A (en) * 1999-02-08 2000-10-24 J. A. Woollam Co. Inc. Compact, high extinction coefficient combination brewster angle and other than brewster angle polarizing system, and method of use
US6141102A (en) * 1999-01-19 2000-10-31 J. A. Woolam Co. Inc Single trianglular shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6169590B1 (en) 1993-12-02 2001-01-02 Ois Optical Imaging Systems, Inc. Liquid crystal display with optical compensator
US6191880B1 (en) 1995-09-23 2001-02-20 Carl-Zeiss-Stiftung Radial polarization-rotating optical arrangement and microlithographic projection exposure system incorporating said arrangement
US6275291B1 (en) * 1998-09-16 2001-08-14 Nanophotonics Ag Micropolarimeter and ellipsometer
US6353477B1 (en) 1992-09-18 2002-03-05 J. A. Woollam Co. Inc. Regression calibrated spectroscopic rotating compensator ellipsometer system with pseudo-achromatic retarder system
US6412989B1 (en) 2000-04-10 2002-07-02 Motorola, Inc. Directable laser transmission module
US20030035191A1 (en) * 2000-01-27 2003-02-20 Franco Moia Optical security device
US6606181B2 (en) * 2000-12-22 2003-08-12 Optellios, Inc. Optical power limiting control
US20030156523A1 (en) * 2002-02-15 2003-08-21 University Of Massachusetts Optical storage system
US6735017B1 (en) * 1997-11-26 2004-05-11 Sharp Kabushiki Kaisha Broadband optical retardation device
US20040120040A1 (en) * 1998-11-13 2004-06-24 Rolic Ag Optical component
US20040174479A1 (en) * 2001-08-29 2004-09-09 Roosendaal Sander Jurgen Arrangements in a transflective liquid crystal display
US20040179158A1 (en) * 2002-01-07 2004-09-16 Eastman Kodak Company Display with a wire grid polarizing beamsplitter
US6816207B2 (en) * 2001-04-27 2004-11-09 Lg.Philips Lcd Co., Ltd. Autostereoscopic display apparatus and method of manufacturing the same
US6900866B2 (en) 2002-01-07 2005-05-31 Eastman Kodak Company Modulation optical system with compensator
US20060082702A1 (en) * 2002-06-28 2006-04-20 Jacobs Adrian M S Optical device and display operating in two dimensional and autostereoscopic three dimensional modes
US20080049321A1 (en) * 2006-08-25 2008-02-28 Jds Uniphase Corporation Passive Depolarizer
CN100470323C (en) * 1997-05-09 2009-03-18 罗利克有限公司 Optical element and anti-fake or anti-copy element including same
US7789515B2 (en) 2007-05-17 2010-09-07 Moxtek, Inc. Projection device with a folded optical path and wire-grid polarizer
US7800823B2 (en) 2004-12-06 2010-09-21 Moxtek, Inc. Polarization device to polarize and further control light
US7813039B2 (en) 2004-12-06 2010-10-12 Moxtek, Inc. Multilayer wire-grid polarizer with off-set wire-grid and dielectric grid
US20110027494A1 (en) * 2007-07-03 2011-02-03 Kim Leong Tan Non-etched flat polarization-selective diffractive optical elements
US7961393B2 (en) 2004-12-06 2011-06-14 Moxtek, Inc. Selectively absorptive wire-grid polarizer
US20110242478A1 (en) * 2008-12-19 2011-10-06 Arisawa Mfg. Co., Ltd. Liquid crystal filter, retardation film, and optical low-pass filter
US20120162765A1 (en) * 2010-12-27 2012-06-28 National Chiao Tung University Photoelectric devices having inhomogeneous polarization selectivity and the manufacturing method thereof
US8248696B2 (en) 2009-06-25 2012-08-21 Moxtek, Inc. Nano fractal diffuser
WO2012139108A1 (en) 2011-04-08 2012-10-11 Dolby Laboratories Licensing Corporation Method and apparatus for flicker reduction and contrast enhancement in 3d displays
US8611007B2 (en) 2010-09-21 2013-12-17 Moxtek, Inc. Fine pitch wire grid polarizer
US20140104402A1 (en) * 2011-05-13 2014-04-17 Écrans Polaires Inc. / Polar Screens Inc. Method and display for concurrently displaying a first image and a second image
USRE44889E1 (en) * 2000-07-15 2014-05-13 F. Poszat Hu, Llc Bistable liquid crystal devices
US8755113B2 (en) 2006-08-31 2014-06-17 Moxtek, Inc. Durable, inorganic, absorptive, ultra-violet, grid polarizer
US8873144B2 (en) 2011-05-17 2014-10-28 Moxtek, Inc. Wire grid polarizer with multiple functionality sections
US8913320B2 (en) 2011-05-17 2014-12-16 Moxtek, Inc. Wire grid polarizer with bordered sections
US8913321B2 (en) 2010-09-21 2014-12-16 Moxtek, Inc. Fine pitch grid polarizer
US8922890B2 (en) 2012-03-21 2014-12-30 Moxtek, Inc. Polarizer edge rib modification
US9135864B2 (en) 2010-05-14 2015-09-15 Dolby Laboratories Licensing Corporation Systems and methods for accurately representing high contrast imagery on high dynamic range display systems
US9348076B2 (en) 2013-10-24 2016-05-24 Moxtek, Inc. Polarizer with variable inter-wire distance
CN106647212A (en) * 2015-11-03 2017-05-10 北京理工大学 Holographic three-dimensional display method and system
US9772530B2 (en) 2010-05-14 2017-09-26 Dolby Laboratories Licensing Corporation High dynamic range displays using filterless LCD(s) for increasing contrast and resolution
US10571762B2 (en) 2010-05-14 2020-02-25 Dolby Laboratories Licensing Corporation High dynamic range displays using filterless LCD(s) for increasing contrast and resolution
US10656596B2 (en) 2014-10-09 2020-05-19 EagleMae Ventures LLC Video display and method providing vision correction for multiple viewers
US10955705B2 (en) * 2017-06-30 2021-03-23 Fujifilm Corporation Wearable display device comprising an optically-anisotropic layer having liquid crystal compounds with optical axes continuously rotating along at least one in-plane direction
US11415728B2 (en) 2020-05-27 2022-08-16 Looking Glass Factory, Inc. System and method for holographic displays

Families Citing this family (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2306231A (en) * 1995-10-13 1997-04-30 Sharp Kk Patterned optical polarising element
JP2000506998A (en) 1996-03-15 2000-06-06 レティナル ディスプレイ ケイマン リミティッド Method and apparatus for viewing images
US5919872A (en) * 1997-06-12 1999-07-06 Shell Oil Company Process for crystallizing blends of polyethylene terephthalate and polyethylene isophthalate
US6055103A (en) * 1997-06-28 2000-04-25 Sharp Kabushiki Kaisha Passive polarisation modulating optical element and method of making such an element
GB9802158D0 (en) * 1997-06-28 1998-04-01 Sharp Kk Method of making a patterned retarder and patterned retarder
GB2331883A (en) * 1997-11-26 1999-06-02 Sharp Kk Dual image viewing system
JP4475813B2 (en) 1998-09-14 2010-06-09 エスビージー・ラボラトリーズ・インコーポレイテッド Holographic illumination device
WO2000023835A1 (en) 1998-10-16 2000-04-27 Digilens, Inc. Holographic technique for illumination of image displays using ambient illumination
WO2000062104A1 (en) * 1998-10-16 2000-10-19 Digilens, Inc. System and method for modulating light intensity
US6421109B1 (en) 1998-10-16 2002-07-16 Digilens, Inc. Method and system for display resolution multiplication
US6678078B1 (en) 1999-01-07 2004-01-13 Digilens, Inc. Optical filter employing holographic optical elements and image generating system incorporating the optical filter
US6504629B1 (en) 1999-03-23 2003-01-07 Digilens, Inc. Method and apparatus for illuminating a display
US6507419B1 (en) 1999-03-23 2003-01-14 Digilens, Inc. Illumination system using optical feedback
US6424437B1 (en) 2000-10-10 2002-07-23 Digilens, Inc. Projection display employing switchable holographic optical elements
KR100603455B1 (en) * 2000-12-30 2006-07-20 엘지.필립스 엘시디 주식회사 Polarizing Stereoscopic Apparatus and Fabricating method thereof
DE102006005860A1 (en) * 2006-02-09 2007-08-30 Bayer Innovation Gmbh Method and device for producing polarization holograms
JP6354106B2 (en) 2012-12-31 2018-07-11 エルジー・ケム・リミテッド Optical element manufacturing method
US10379495B2 (en) * 2017-01-12 2019-08-13 Ziel Optics, Inc. Gun sight with brightness control

Citations (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA475049A (en) * 1951-07-03 Dreyer Laboratories Polarizers
US2647440A (en) * 1947-08-08 1953-08-04 Miles P Rehorn Molecularly aligned sheet material
US3437401A (en) * 1964-05-25 1969-04-08 Visorama Printed Motions Co Light-intercepting sheet for an illuminated display device
US3601469A (en) * 1969-08-11 1971-08-24 Anthony Siksai Rotary polarizer
US3825316A (en) * 1972-04-24 1974-07-23 Rca Corp Apparatus for providing an optical system using adaptive holographic components
US4114990A (en) * 1976-05-04 1978-09-19 International Standard Electric Corporation Liquid crystal rotator
GB1534456A (en) * 1977-10-11 1978-12-06 Standard Telephones Cables Ltd Optical scanning device
US5020882A (en) * 1987-11-06 1991-06-04 Makow David M Electro-optic animated displays and indicators
EP0449164A2 (en) * 1990-03-26 1991-10-02 Matsushita Electric Industrial Co., Ltd. Method for forming a computer generated hologram
EP0450644A2 (en) * 1990-04-06 1991-10-09 Matsushita Electric Industrial Co., Ltd. A liquid crystal spacial light modulator and a holographic image information recording apparatus using the same
EP0451681A2 (en) * 1990-04-05 1991-10-16 Seiko Epson Corporation Optical apparatus
US5121235A (en) * 1988-12-21 1992-06-09 International Business Machines Corporation Liquid crystal display device having light transmission control layer
GB2250605A (en) * 1990-12-03 1992-06-10 Raytheon Co Two-dimensional, phased-array optical beam steerer
US5235449A (en) * 1990-03-02 1993-08-10 Hitachi, Ltd. Polarizer with patterned diacetylene layer, method for producing the same, and liquid crystal display device including such polarizer
US5243455A (en) * 1990-05-11 1993-09-07 The University Of Colorado Foundation, Inc. Chiral smectic liquid crystal polarization interference filters
US5327285A (en) * 1990-06-11 1994-07-05 Faris Sadeg M Methods for manufacturing micropolarizers
US5381253A (en) * 1991-11-14 1995-01-10 Board Of Regents Of University Of Colorado Chiral smectic liquid crystal optical modulators having variable retardation
US5434687A (en) * 1993-03-15 1995-07-18 Kabushiki Kaisha Toshiba Liquid crystal display device having polarization areas or orientation areas in radial or concentric ring pattern

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA2036435A1 (en) * 1990-03-26 1991-09-27 Paul J. Anderson Reagent unit

Patent Citations (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA475049A (en) * 1951-07-03 Dreyer Laboratories Polarizers
US2647440A (en) * 1947-08-08 1953-08-04 Miles P Rehorn Molecularly aligned sheet material
US3437401A (en) * 1964-05-25 1969-04-08 Visorama Printed Motions Co Light-intercepting sheet for an illuminated display device
US3601469A (en) * 1969-08-11 1971-08-24 Anthony Siksai Rotary polarizer
US3825316A (en) * 1972-04-24 1974-07-23 Rca Corp Apparatus for providing an optical system using adaptive holographic components
US4114990A (en) * 1976-05-04 1978-09-19 International Standard Electric Corporation Liquid crystal rotator
GB1534456A (en) * 1977-10-11 1978-12-06 Standard Telephones Cables Ltd Optical scanning device
US5020882A (en) * 1987-11-06 1991-06-04 Makow David M Electro-optic animated displays and indicators
US5122890A (en) * 1987-11-06 1992-06-16 Makow David M Electro-optic animated displays and indicators employing electro-optical cells and mosaic segment polarizer
US5121235A (en) * 1988-12-21 1992-06-09 International Business Machines Corporation Liquid crystal display device having light transmission control layer
US5235449A (en) * 1990-03-02 1993-08-10 Hitachi, Ltd. Polarizer with patterned diacetylene layer, method for producing the same, and liquid crystal display device including such polarizer
EP0449164A2 (en) * 1990-03-26 1991-10-02 Matsushita Electric Industrial Co., Ltd. Method for forming a computer generated hologram
EP0451681A2 (en) * 1990-04-05 1991-10-16 Seiko Epson Corporation Optical apparatus
EP0450644A2 (en) * 1990-04-06 1991-10-09 Matsushita Electric Industrial Co., Ltd. A liquid crystal spacial light modulator and a holographic image information recording apparatus using the same
US5243455A (en) * 1990-05-11 1993-09-07 The University Of Colorado Foundation, Inc. Chiral smectic liquid crystal polarization interference filters
US5327285A (en) * 1990-06-11 1994-07-05 Faris Sadeg M Methods for manufacturing micropolarizers
GB2250605A (en) * 1990-12-03 1992-06-10 Raytheon Co Two-dimensional, phased-array optical beam steerer
US5381253A (en) * 1991-11-14 1995-01-10 Board Of Regents Of University Of Colorado Chiral smectic liquid crystal optical modulators having variable retardation
US5434687A (en) * 1993-03-15 1995-07-18 Kabushiki Kaisha Toshiba Liquid crystal display device having polarization areas or orientation areas in radial or concentric ring pattern

Non-Patent Citations (14)

* Cited by examiner, † Cited by third party
Title
O Brien et al, Generalised Dynamic Holographic Interconnects Using Spatial Light Modulators, Mar. 1993, vol. 6, Technical Digest Series; OSA Meeting for Spatial Light Modulators and Applications. *
O'Brien et al, "Generalised Dynamic Holographic Interconnects Using Spatial Light Modulators," Mar. 1993, vol. 6, Technical Digest Series; OSA Meeting for Spatial Light Modulators and Applications.
Optical Computing, Palm Springs 1993, Technical Digest vol. 7, Opt. Soc. America, Mar. 1993, J. Ford et al., "Polarization-Selective Computer-Generated Holograms For Optical Multistage Interconnection Networks", pp. 258-261.
Optical Computing, Palm Springs 1993, Technical Digest vol. 7, Opt. Soc. America, Mar. 1993, J. Ford et al., Polarization Selective Computer Generated Holograms For Optical Multistage Interconnection Networks , pp. 258 261. *
Optics Letters, vol. 16, No. 18, Sep. 15, 1991, Hirofumi Yamakazi et al., "4×4 Free-Space Optical Switching Using Real-Time Binary Phase-Only Holograms Generated By A Liquid-Crystal Display", pp. 1415-1417.
Optics Letters, vol. 16, No. 18, Sep. 15, 1991, Hirofumi Yamakazi et al., 4 4 Free Space Optical Switching Using Real Time Binary Phase Only Holograms Generated By A Liquid Crystal Display , pp. 1415 1417. *
Optics Letters, vol. 17, No. 11, Jun. 1992, Masayuki Kato et al., "Multichannel Optical Switch That Uses Holograms", pp. 769-771.
Optics Letters, vol. 17, No. 11, Jun. 1992, Masayuki Kato et al., Multichannel Optical Switch That Uses Holograms , pp. 769 771. *
Optics Letters, vol. 18, No. 6, Mar. 15, 1993, Joseph E. Ford et al., "Polarization-Selective Computer-Generated Holograms", pp. 456-458.
Optics Letters, vol. 18, No. 6, Mar. 15, 1993, Joseph E. Ford et al., Polarization Selective Computer Generated Holograms , pp. 456 458. *
Schadt et al, "Surface-Induced Parallel Alignment of Liquid Crystals by Linearly Polymerized Photopolymers", Jpn. J. Appl. Phys., vol. 31 (Jul. 1992) pp. 2155-2164.
Schadt et al, Surface Induced Parallel Alignment of Liquid Crystals by Linearly Polymerized Photopolymers , Jpn. J. Appl. Phys., vol. 31 (Jul. 1992) pp. 2155 2164. *
Yakolev et al, "New Concept to Achieve Color LCD's with Linearly Photo-polymerized (LPP) LCD-Substrates," Aug.-Sep. 1993, SID. Euro Display '93, Strasbourg.
Yakolev et al, New Concept to Achieve Color LCD s with Linearly Photo polymerized (LPP) LCD Substrates, Aug. Sep. 1993, SID. Euro Display 93, Strasbourg. *

Cited By (74)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5784139A (en) * 1991-07-26 1998-07-21 Rolic Ag Image display device
US6353477B1 (en) 1992-09-18 2002-03-05 J. A. Woollam Co. Inc. Regression calibrated spectroscopic rotating compensator ellipsometer system with pseudo-achromatic retarder system
US6169590B1 (en) 1993-12-02 2001-01-02 Ois Optical Imaging Systems, Inc. Liquid crystal display with optical compensator
US6885502B2 (en) 1995-09-23 2005-04-26 Carl-Zeiss-Stiftung Radial polarization-rotating optical arrangement and microlithographic projection exposure system incorporating said arrangement
US20020126380A1 (en) * 1995-09-23 2002-09-12 Carl-Zeiss-Stiftung Radial polarization-rotating optical arrangement and microlithographic projection exposure system incorporating said arrangement
US6392800B2 (en) 1995-09-23 2002-05-21 Carl-Zeiss-Stiftung Radial polarization-rotating optical arrangement and microlithographic projection exposure system incorporating said arrangement
US6191880B1 (en) 1995-09-23 2001-02-20 Carl-Zeiss-Stiftung Radial polarization-rotating optical arrangement and microlithographic projection exposure system incorporating said arrangement
US5745203A (en) * 1996-03-28 1998-04-28 Motorola, Inc. Liquid crystal display device including multiple ambient light illumination modes with switchable holographic optical element
CN100470323C (en) * 1997-05-09 2009-03-18 罗利克有限公司 Optical element and anti-fake or anti-copy element including same
US6735017B1 (en) * 1997-11-26 2004-05-11 Sharp Kabushiki Kaisha Broadband optical retardation device
US5963325A (en) * 1997-12-23 1999-10-05 J.A. Woollam Co. Inc. Dual vertically oriented triangular shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US5946098A (en) * 1997-12-23 1999-08-31 J.A. Woollam Co. Inc. Optical elements for use in spectroscopic ellipsometer and polarimeter systems
US6275291B1 (en) * 1998-09-16 2001-08-14 Nanophotonics Ag Micropolarimeter and ellipsometer
US20070035833A1 (en) * 1998-11-13 2007-02-15 Rolic Ag Optical component
US20040120040A1 (en) * 1998-11-13 2004-06-24 Rolic Ag Optical component
US7375888B2 (en) 1998-11-13 2008-05-20 Rolic Ltd Optical component
US6118537A (en) * 1999-01-04 2000-09-12 J. A. Woollam Co. Inc. Multiple tipped berek plate optical retarder elements for use in spectroscopic ellipsometer and polarimeter systems
US6100981A (en) * 1999-01-04 2000-08-08 J.A. Woollam Co. Inc. Dual horizontally oriented triangle shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6084674A (en) * 1999-01-04 2000-07-04 J. A. Woollam Co., Inc. Parallelogram shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6141102A (en) * 1999-01-19 2000-10-31 J. A. Woolam Co. Inc Single trianglular shaped optical retarder element for use in spectroscopic ellipsometer and polarimeter systems
US6137618A (en) * 1999-02-08 2000-10-24 J. A. Woollam Co. Inc. Compact, high extinction coefficient combination brewster angle and other than brewster angle polarizing system, and method of use
US20030035191A1 (en) * 2000-01-27 2003-02-20 Franco Moia Optical security device
US6806930B2 (en) * 2000-01-27 2004-10-19 Rolic Ag Optical security device
US6412989B1 (en) 2000-04-10 2002-07-02 Motorola, Inc. Directable laser transmission module
USRE44889E1 (en) * 2000-07-15 2014-05-13 F. Poszat Hu, Llc Bistable liquid crystal devices
US6606181B2 (en) * 2000-12-22 2003-08-12 Optellios, Inc. Optical power limiting control
US6816207B2 (en) * 2001-04-27 2004-11-09 Lg.Philips Lcd Co., Ltd. Autostereoscopic display apparatus and method of manufacturing the same
US7339643B2 (en) * 2001-08-29 2008-03-04 Koninklijke Philips Electronics N.V. Arrangements in a transflective liquid crystal display
US20040174479A1 (en) * 2001-08-29 2004-09-09 Roosendaal Sander Jurgen Arrangements in a transflective liquid crystal display
US20050128392A1 (en) * 2002-01-07 2005-06-16 Kurtz Andrew F. Exposure system for creating a patterned polarization compensator
US6982773B2 (en) 2002-01-07 2006-01-03 Moxtek, Inc. Exposure system for creating a patterned polarization compensator
US7023512B2 (en) 2002-01-07 2006-04-04 Moxtek, Inc. Spatially patterned polarization compensator
US6900866B2 (en) 2002-01-07 2005-05-31 Eastman Kodak Company Modulation optical system with compensator
US7061561B2 (en) 2002-01-07 2006-06-13 Moxtek, Inc. System for creating a patterned polarization compensator
US20040179158A1 (en) * 2002-01-07 2004-09-16 Eastman Kodak Company Display with a wire grid polarizing beamsplitter
US7507504B2 (en) 2002-02-15 2009-03-24 University Of Massachusetts Optical storage system
US20030156523A1 (en) * 2002-02-15 2003-08-21 University Of Massachusetts Optical storage system
US20060082702A1 (en) * 2002-06-28 2006-04-20 Jacobs Adrian M S Optical device and display operating in two dimensional and autostereoscopic three dimensional modes
US7580085B2 (en) * 2002-06-28 2009-08-25 Sharp Kabushiki Kaisha Optical device and display operating in two dimensional and autostereoscopic three dimensional modes
US7961393B2 (en) 2004-12-06 2011-06-14 Moxtek, Inc. Selectively absorptive wire-grid polarizer
US7800823B2 (en) 2004-12-06 2010-09-21 Moxtek, Inc. Polarization device to polarize and further control light
US7813039B2 (en) 2004-12-06 2010-10-12 Moxtek, Inc. Multilayer wire-grid polarizer with off-set wire-grid and dielectric grid
US8027087B2 (en) 2004-12-06 2011-09-27 Moxtek, Inc. Multilayer wire-grid polarizer with off-set wire-grid and dielectric grid
US20080049321A1 (en) * 2006-08-25 2008-02-28 Jds Uniphase Corporation Passive Depolarizer
US8755113B2 (en) 2006-08-31 2014-06-17 Moxtek, Inc. Durable, inorganic, absorptive, ultra-violet, grid polarizer
US7789515B2 (en) 2007-05-17 2010-09-07 Moxtek, Inc. Projection device with a folded optical path and wire-grid polarizer
US20110027494A1 (en) * 2007-07-03 2011-02-03 Kim Leong Tan Non-etched flat polarization-selective diffractive optical elements
US8643822B2 (en) 2007-07-03 2014-02-04 Jds Uniphase Corporation Non-etched flat polarization-selective diffractive optical elements
US20110242478A1 (en) * 2008-12-19 2011-10-06 Arisawa Mfg. Co., Ltd. Liquid crystal filter, retardation film, and optical low-pass filter
US8248696B2 (en) 2009-06-25 2012-08-21 Moxtek, Inc. Nano fractal diffuser
US10571762B2 (en) 2010-05-14 2020-02-25 Dolby Laboratories Licensing Corporation High dynamic range displays using filterless LCD(s) for increasing contrast and resolution
US9864243B2 (en) 2010-05-14 2018-01-09 Dolby Laboratories Licensing Corporation High dynamic range displays using filterless LCD(s) for increasing contrast and resolution
US9772530B2 (en) 2010-05-14 2017-09-26 Dolby Laboratories Licensing Corporation High dynamic range displays using filterless LCD(s) for increasing contrast and resolution
US9135864B2 (en) 2010-05-14 2015-09-15 Dolby Laboratories Licensing Corporation Systems and methods for accurately representing high contrast imagery on high dynamic range display systems
US8611007B2 (en) 2010-09-21 2013-12-17 Moxtek, Inc. Fine pitch wire grid polarizer
US8913321B2 (en) 2010-09-21 2014-12-16 Moxtek, Inc. Fine pitch grid polarizer
US20120162765A1 (en) * 2010-12-27 2012-06-28 National Chiao Tung University Photoelectric devices having inhomogeneous polarization selectivity and the manufacturing method thereof
CN102565910A (en) * 2010-12-27 2012-07-11 财团法人交大思源基金会 Optical element with non-uniform polarization selectivity and method of making the same
WO2012139108A1 (en) 2011-04-08 2012-10-11 Dolby Laboratories Licensing Corporation Method and apparatus for flicker reduction and contrast enhancement in 3d displays
US9955145B2 (en) * 2011-04-08 2018-04-24 Dolby Laboratories Licensing Corporation Method and apparatus for flicker reduction and contrast enhancement in 3D displays
US20140028815A1 (en) * 2011-04-08 2014-01-30 Dolby Laboratories Licensing Corporation Method and Apparatus for Flicker Reduction and Contrast Enhancement in 3D Displays
US9407907B2 (en) * 2011-05-13 2016-08-02 Écrans Polaires Inc./Polar Screens Inc. Method and display for concurrently displaying a first image and a second image
US20140104402A1 (en) * 2011-05-13 2014-04-17 Écrans Polaires Inc. / Polar Screens Inc. Method and display for concurrently displaying a first image and a second image
US8913320B2 (en) 2011-05-17 2014-12-16 Moxtek, Inc. Wire grid polarizer with bordered sections
US8873144B2 (en) 2011-05-17 2014-10-28 Moxtek, Inc. Wire grid polarizer with multiple functionality sections
US8922890B2 (en) 2012-03-21 2014-12-30 Moxtek, Inc. Polarizer edge rib modification
US9354374B2 (en) 2013-10-24 2016-05-31 Moxtek, Inc. Polarizer with wire pair over rib
US9632223B2 (en) 2013-10-24 2017-04-25 Moxtek, Inc. Wire grid polarizer with side region
US9348076B2 (en) 2013-10-24 2016-05-24 Moxtek, Inc. Polarizer with variable inter-wire distance
US10656596B2 (en) 2014-10-09 2020-05-19 EagleMae Ventures LLC Video display and method providing vision correction for multiple viewers
CN106647212A (en) * 2015-11-03 2017-05-10 北京理工大学 Holographic three-dimensional display method and system
CN106647212B (en) * 2015-11-03 2019-06-04 北京理工大学 A kind of hologram three-dimensional display methods and system
US10955705B2 (en) * 2017-06-30 2021-03-23 Fujifilm Corporation Wearable display device comprising an optically-anisotropic layer having liquid crystal compounds with optical axes continuously rotating along at least one in-plane direction
US11415728B2 (en) 2020-05-27 2022-08-16 Looking Glass Factory, Inc. System and method for holographic displays

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EP0664495B1 (en) 2002-04-03
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JPH07210069A (en) 1995-08-11
DE69526134T3 (en) 2004-05-06

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